Method of processing a digital signal derived from an analog input signal of a GNSS receiver, a GNSS receiver base band circuit for carrying out the method and a GNSS receiver

ABSTRACT

For suppression of continuous wave interferers at, e.g., up to four interferer frequencies (f 1 , f 2 , f 3 , f 4 ) in a GNSS receiver base band circuit a raw digital signal is, in a band stop unit ( 21 ), shifted, by a first mixer ( 31   a ), by the negative of the first interferer frequency (f 1 ) in the frequency domain whereupon the continuous wave interferer is suppressed by a band stop filter ( 30   a ), a linear phase FIR filter with a suppression band centered at zero, e.g., a filter subtracting a mean over previous subsequent signal values from the actual signal value. After further shifting of the shifted digital signal by the negative of the difference between the second interferer frequency (f 2 ) and the first interferer frequency (f 1 ) the shifted digital signal is again filtered by an identical band stop filter ( 30   b ) and so on. After the last filtering step the shifted digital signal is shifted back to its original position in the frequency domain to provide a filtered digital signal which corresponds to the raw digital signal with narrow interferer bands centered at the interferer frequencies (f 1 , f 2 , f 3 , f 4 ) suppressed.

FIELD OF THE INVENTION

The invention concerns a method for processing a digital signal derived from an analog input signal of a GNSS receiver which contains signals emitted by satellites of GNSS (Global Navigation Satellite System) positioning systems like GPS, GLONASS and GALILEO in order to determine a position. The invention also concerns a base band circuit for carrying out the method and a GNSS receiver comprising such base band circuit.

PRIOR ART

It is well known in the art to suppress continuous wave interferers using so-called notch filters. Digital filters of this type can be controlled in such a way that they suppress a very narrow frequency band centered at a variable suppression frequency which is controlled according to the result of a frequency analysis of a raw, unfiltered digital signal so as to essentially coincide with the interferer frequency. The transfer function in the frequency domain has a zero at the suppression frequency and a pole close by. A system of this kind is described in US 2003/0 112 905 A1.

A notch filter of this type is an IIR filter exhibiting large variations of the group delay in the vicinity of the suppressed interferer frequency. As a consequence frequency components of the raw digital signal which belong to different parts of its frequency band are subjected to widely varying delays and the band stop filtered digital signal is considerably distorted. In a subsequent tracking step where correlations of the band stop filtered signal with sequences characteristic of individual satellites are calculated and the phases of individual satellite signals contained therein are determined this will lead to distorted and generally less pronounced correlation peaks. This may significantly reduce positioning accuracy.

SUMMARY OF THE INVENTION

It is an object of the invention to provide a method of the generic type whereby continuous wave interferers are removed from the digital input signal by band stop filters with fixed suppression frequencies. This object is achieved by the features in the characterizing portion of claim 1.

The method according to the invention provides for reliable suppression of continuous wave interferers while at the same time allowing to pursue additional goals like avoidance of distortions of the digital signal in the band stop filtering step which might compromise positioning accuracy. The method can be carried out in ways which require only very moderate processing capacity for the band stop filtering step. As a consequence, the band stop filtering unit contributes only minimally to hardware complexity and expenses related thereto.

It is a further object of the invention to provide a base band circuit for carrying out the method and a GNSS receiver comprising such base band circuit. The base band circuit and GNSS receiver according to the invention are relatively simple and easy to produce while at the same time offering high positioning accuracy and robustness against jamming signals.

BRIEF DESCRIPTION OF THE DRAWINGS

In the following the invention is described in more detail with reference to drawings showing an embodiment of the invention where

FIG. 1 shows a radio frequency circuit of a GNSS receiver according to the invention,

FIG. 2 shows a base band circuit of a GNSS receiver according to the invention,

FIG. 3 shows a band stop unit of the base band circuit of FIG. 2 and

FIG. 4 shows a band stop filter of the band stop unit of FIG. 3.

DESCRIPTION OF THE PREFERRED EMBODIMENTS

The embodiment described in the following is a receiver suitable for GPS. However, the modfications which are necessary if other systems like GALILEO or GLONASS are to be used are straightforward. The receiver comprises (FIG. 1) an antenna 1 followed by a radio frequency circuit 2, a bandpass filter 3, a TCXO (temperature compensated crystal oscillator) 4 and (FIG. 2) a base band circuit 5. It is advantageous to implement the radio frequency circuit 2 and the base band circuit 5 each on a separate semiconductor chip but other solutions are also possible.

The bandpass filter 3, usually an SAW (surface acoustic wave) filter, is a component external to the radio frequency circuit 2. The TCXO 4, also a separate component, provides a basic frequency of between 19 MHz and 40 MHz, e.g., 26 MHz, which is fed to the radio frequency circuit 2 and further to the base band circuit 5. In the radio frequency circuit 2 the output signal of TCXO 4 controls a PLL unit 6 which produces a 3′158 MHz clock signal from which two further clock signals with half the clock rate, i.e., 1′579 MHz, are derived with one of the clock signals phase-shifted by 90° with respect to the other.

The antenna input of the radio frequency circuit 2 is followed by a low noise amplifier 7 which is connected, via the external band pass filter 3 and a controllable RF amplifier 8, to mixers 9 a,b which also receive the clock signals from PLL unit 6. Together they form a complex mixer which provides an I and Q component of a complex analog signal shifted down to an intermediate frequency of approximately 3 MHz. They are each followed by a high pass filter 10 a;b with a cutoff frequency of about 20 kHz and a controllable low pass filter 11 a;b with a cutoff frequency of around 7.5 MHz connected to the output of the radio frequency circuit 2 via programmable gain amplifiers 12 a;b.

The output of radio frequency circuit 2 is connected to an input of the base band circuit 5. The output signal of TCXO 4 is, via radio frequency circuit 2, also fed to the base band circuit 5 where it controls a PLL unit 13 producing a clock signal with a clock rate of 96 MHz which is reduced to 24 MHz by a subsequent frequency divider 14. Directly at the input of the base band circuit 5 A/D converters 15 a,b with 5 bit resolutions are provided for sampling the input signal with a sampling rate of 24 MHz, producing a complex digital signal which is fed to a complex digital mixer 16 that reduces it to base band and to frequency analyzers 17 a,b whose outputs are connected to a control unit 18 which controls low pass filters 11 a,b in radio frequency circuit 2. The mixer 16 is followed by decimation filters 19 a,b, each with a cut-off frequency of 3 MHz, and down-samplers 20 a;b. A/D converters 15 a,b, mixer 16, frequency analyzers 17 a,b, decimation filters 19 a,b and down-samplers 20 a,b are controlled by the clock signal from frequency divider 14.

A band stop unit 21 for filtering a raw digital signal by removing continuous wave signals and a decimator 22 for reducing the filtered digital signal from 6 to 3 bits are followed by a frequency analyzer 23 whose output signal is used by control unit 18 to control the band stop unit 21 and, via down-samplers 24 a,b, by an acquisition unit 25 for identifying components of the signal as emitted by specific satellites of the GNSS system as well as by a tracking unit 26 for continually tracking the said signal components and analyzing their time delays and for extracting data bits from them.

A frequency divider 27 produces, from the 24 MHz signal output of frequency divider 14, a 8 MHz clock signal which controls band stop unit 21, decimator 22, frequency analyzer 23, down-samplers 24 a,b and tracking unit 26. A further frequency divider 28 provides a 2 MHz clock signal for the acquisition unit 25 which also receives the 96 MHz clock signal from PLL unit 13. The control unit 18 receives data from the tracking unit 25 which, apart from the time delays of signals emitted by the individual satellites, comprise almanac and ephemeris data extracted from the said signals. From those data the control unit 18 calculates the position of the GNSS receiver. The calculations which may also involve additional data stored in the receiver or transmitted to it via some additional link are carried out in ways well known in the art. The control unit 18 also controls the acquisition unit 25 and the tracking unit 26.

After the analog signal received by the antenna 1 (FIG. 1) has been amplified by low noise amplifier 7 its spectrum is reduced to a 30 MHz band centered at the GPS frequency of 1′575.42 MHz by band pass filter 3. After further amplification and mixing any DC component is removed by high pass filters 10 a,b and high frequencies are suppressed by low pass filters 11 a,b for anti-aliasing. The low pass filters 11 a,b are controlled by the control unit 18 (FIG. 2) based on the outputs of frequency analyzers 17 a;b in such a way that the signal is, with respect to the signal at a reference frequency of 3 MHz, attenuated by not more than −3 dB at 7.5 MHz and by at least −12 dB at 12 MHz, i.e., at half the sampling rate of A/D converters 15 a,b at the input of base band circuit 5. The programmable gain amplifiers 12 a,b adjust the signal to the input range of the A/D converters 15 a,b.

The amplified and filtered complex analog signal is then converted to a complex digital signal by A/D converters 15 a,b of base band circuit 5 and then derotated, i.e., shifted essentially to zero by complex digital mixer 16. After its spectrum has been reduced to a 3 MHz frequency band by decimation filters 19 a,b, its sampling rate is reduced to 8MHz by down-samplers 20 a;b. This raw digital signal which is restricted to a fixed raw signal frequency band extending from −3 MHz to +3 MHz is then fed to band stop unit 21 for filtering. Several continuous wave interferers can be suppressed with only negligible distortion of the raw digital signal to produce a filtered digital signal restricted to a filtered signal frequency band which coincides with the raw signal frequency band as will be explained in more detail below. In a next step the filtered digital signal is requantized from 6 bits to 3 bits in the decimator 22 which uses a non-linear decimation table. The resulting digital signal is then fed in parallel to frequency analyzer 23, tracking unit 26 and, via down-samplers 24 a,b which reduce the sample frequency to 2 MHz, to acquisition unit 25.

In the acquisition unit 25 a signal derived from this input signal is correlated with internally produced characteristic sequences of GNSS satellites at various Doppler frequencies and with various phase shifts. The relatively low 2 MHz sample frequency allows efficient processing of the signal and, as a consequence, fast lock-on to received satellite signals.

On the other hand, in the tracking unit 26, where the same sequences, frequencies and phase shifts are applied as have yielded high correlation values in the acquisition unit 25, the higher sample frequency of 8 MHz allows for a very precise determination of the positions of the correlation peaks and associated phases of the said satellite signals which in turn allows a precise calculation of receiver position. The results from frequency analyzer 23 which may be a part of the tracking circuit 26 using channels with varying scanning frequencies and constant sequences, are employed for the detection of any continuous wave interferers and determination of their interferer frequencies which are then used by the control unit 18 for controlling band stop unit 21 in such a way that the interferer frequencies are suppressed. The interferer frequencies can be identified by cyclical sweeping through the raw signal frequency band in steps of, e.g., 1 kHz and comparing the individual energy densities with a mean over the entire frequency band.

In the following, band stop unit 21 is explained in more detail with reference to FIG. 3. It comprises a series of several—in the example five—complex digital mixers 29 a,b,c,d,e. With the exception of a last mixer 29 e each of them is followed by a complex digital band stop filter 30 a;b;c;d. Each of the mixers 29 a,b,c,d,e is directly controlled by a numerically controlled oscillator 31 a;b;c;d;e locked to the 8 MHz clock signal from frequency divider 27. Mixer 29 a, band stop filter 30 a and oscillator 31 a form a band stop subunit suitable for suppressing a single continuous wave interferer. The same applies to mixers 29 b,c,d, band stop filters 30 b;c;d and oscillators 31 b;c;d. The band stop filters 30 a,b,c,d are preferably equal, conforming to a band stop filter which exhibits at any time high attenuation in a suppression band centered at a fixed suppression frequency—normally but not necessarily zero—while the frequency response is essentially constant over the relevant frequency band outside the suppression band. The mixers 29 a,b,c,d,e are also equal.

The mixers 29 a,b,c,d are controlled by oscillators 31 a;b;c;d in such a way that each of them provides a shifted digital signal to the subsequent band stop filter 30 a;b;c;d. Oscillators 31 a,b,c,d are each controlled by control unit 18 via a frequency input line delivering a frequency signal while oscillators 31 b,c,d,e each receive a phase signal from the previous oscillator 31 a;b;c;d.

It has been found to be advantageous if time-shifts between contributions of different frequency components of the raw digital signal which are fed to the band stop filter unit 21 to the filtered digital signal at its output do not differ, at least not by more than half a sampling interval. If this condition is not fulfilled the filtered digital signal will be distorted. As a consequence, the correlation results derived in the following tracking step will be distorted in turn and the correlation peaks generally less pronounced. This may lead to a misreading of the correlation signals and introduce relatively large errors into the determination of the phases of the satellite signals which will be reflected in a decrease of positioning accuracy.

If the band stop filter is time invariant a transfer function can be defined with a frequency response and a phase response and the above condition can be reformulated as a condition on the group delay, i.e., the negative of the derivative of the phase response. The group delay ought to not vary by more than half the length of the sampling interval, i.e., in the present case, where the sampling freqency is 8 MHz, by not more than 67.5 ns.

This condition is, of course, always fulfilled if the group delay is constant, i.e., if the phase response is linear. As is well known in the art, this is the case with linear phase FIR filters. A suitable example of a band stop filter of this type which suppresses a stop band centered at zero is a filter which subtracts a gliding mean from the signal in the time domain, i.e., where the value of the output signal as a function of time t is

y(n)=x(n)−1/M×[x(n−k ₀)+x((n−1)−k)+ . . . +x((n−M+1)−k ₀)]  (1)

for nT≦t<(n+1)T with T the length of the sample interval and x(k) the value of the input signal at time t for kT≦t<(k+1)T. M can be any positive integer, preferably between 250 and 70′000, e.g., 2′046. It may also vary depending on the desired width of the suppression band. k₀≧0 signifies a delay of the gliding mean with respect to the input signal by k₀T.

The fact that the calculation of the gliding mean requires relatively high processing and memory capacity precludes its application in many cases. However, calculation of the gliding mean can be replaced by an integrate and dump process where the term subtracted from the actual value of the input signal is a mean taken over a series of subsequent values of the input signal which has a fixed length M, which mean is replaced after a period of length MT, i.e.,

y(n)=x(n)−1/M×[x(1M−k ₀)+x(1M−k ₀−1)+ . . . +x((1−1)M−k ₀+1)] with 1 such that 1M≦n<(1+1)M   (2)

again with k₀≧0. Preferably, k₀ is equal to zero or to a small positive integer.

This band stop filter is not time invariant but can be seen as a collection of M different time invariant filters which are applied in turn, depending on the value of n mod M. Each of those filters subtracts a gliding mean delayed by (n mod M)+k₀ from the signal. The filter therefore approximates a band stop filter according to (1) whereas its requirements concerning processing and memory capacity are far smaller.

Each of the band stop filters 30 a,b,c,d comprises (FIG. 4) a processing unit 32 which calculates a processed digital signal from the shifted digital signal at its input. In the example the processed digital signal is a mean produced by adding up the values of M subsequent samples of the shifted digital signal and dividing the sum by M, which is then stored and output by the processing unit 32 until a new mean of the next M values of samples has been calculated by which it is replaced. In an adder 33 the value of the actual sample of the processed digital signal, i.e., the actually stored mean, is subtracted from the value of the actual sample of the shifted digital signal, x(n). So each of the band stop filters 30 a,b,c,d carries out the process according to (2), suppressing a narrow suppression band of the shifted digital signal which is centered at zero frequency. The suppression is effected in such a way that the delay of frequency components in the relevant frequency band varies only negligibly as a function of the frequency.

The function of the band stop unit 21 as a whole is explained in the following. If, e.g., three continuous wave interferers at interferer frequencies f₁<f₂<f₃ have been detected the first interferer frequency f₁ is fed to the first oscillator 31 a which produces a phase signal −f₁t (mod 1) from which a complex exponential e^(2njf)1^(t) is then derived and fed to mixer 29 a which accordingly shifts the raw digital signal at the input of the band stop unit 21 in the frequency domain by by −f1. After that, band stop filter 30 a suppresses a fixed frequency component of the shifted digital signal, namely a suppression band centered at a suppression frequency which is equal to zero, i.e., situated at frequency f₁ in relation to the raw digital signal fed to band stop unit 21.

In an essentially analogous manner oscillator 31 b, controlled by the frequency signal on the frequency input line and the phase signal from oscillator 31 a, produces a phase signal −f₂t from which the phase signal −f₁t from oscillator 31 a is subtracted. This results in a phase difference signal (f₁−f₂)t from which complex exponential e^(2nj(f) ₂ ^(−f) ₁ ^()t) is derived and fed to mixer 29 b. The latter therefore shifts the shifted digital signal further in the frequency domain by f₁−f₂, that is, by −f₂ in relation to the input signal of band stop unit 21. Again, band stop filter 30 b acts on the signal in the same manner as previous band stop filter 30 a, suppressing a narrow suppression band centered at zero frequency, corresponding to frequency f₂ in the raw digital signal at the input of band stop unit 21.

In exactly the same manner, oscillator 31 c produces a phase signal −f₃t, a phase difference signal (f₂−f₃)t and a complex exponential e^(2nj(f) ₃ ^(−f) ₂ ^()t) which is fed to mixer 29 c which further shifts the shifted digital signal by f₂−f₃ such that it is now in total shifted by −f₃ in the frequency domain with respect to the raw digital signal. Having been filtered by band stop filter 30 c it reaches mixer 29 d and band stop filter 30 d. As there are at the moment only three interfering signals which need to be suppressed band stop filter 30 d is inactive and f₄=0. Oscillator 31 d accordingly produces a phase signal of zero and a phase difference signal of f₃t from which a complex explonential e^(2njf)3^(t) is derived. Mixer 31 d therefore shifts the shifted digital signal by −f₃, that is, to a filtered signal frequency band which coincides with the raw signal frequency band, i.e., the shifted digital signal is shifted back to its original position in the frequency domain, but with narrow interferer bands centered at the interferer frequencies f₁, f₂ and f₃ of the continuous wave interferers suppressed.

The last oscillator 31 e does not produce a phase signal of its own but only receives the phase signal from previous oscillator 31 d, inverts it and then derives a complex exponential in the same way as the previous oscillators 31 b,c,d, i.e., the effect is the same as when the previous oscillators 31 b,c,d receive a frequency signal indicating f=0 from control unit 18. As in the present case it has been assumed that f₄=0 the frequency difference is also zero and the complex exponential equals one, i.e., mixer 29 e is inactive. However, if f₄≠0 then oscillator 31 d operates exactly like oscillators 31 b,c, producing a phase signal −f₄t, a phase difference signal (f₃−f₄)t and a complex exponential e^(2nj(f) ₄ ^(−f) ₃ ^()t). Oscillator 31 e then receives a phase signal −f₄t from oscillator 31 d, inverts it to f₄t and produces a complex exponential e^(−2njf) ₄ ^(t) which shifts the digital signal to the filtered signal frequency band, that is, in the present example, to its original position in the frequency domain.

In the example, the band stop filters 30 a,b,c,d are equal, with suppression frequencies equal to zero. Moreover, they are fixed, i.e., time independent, if not on the scale of the sampling interval T as, e.g., a gliding mean according to (1) would be, then at least on the coarser time scale given by the multiple MT of the sampling interval T. As the frequency band is shifted in such a way that each of the interferer frequencies of the shifted digital signal coincides with the suppression frequency in one of the band stop filters 30 a,b,c,d it is, in particular, unnecessary to keep the suppression frequency variable. This allows for implementation of the filter in a very simple and efficient way and for pursuing other advantages. In particular, it is comparatively easy to achieve very low limits on the variability of group delay or to practically exclude such variability altogether, using a linear phase FIR filter or, as in the example, a collection of such filters which are employed in turn.

Many deviations from the example given are, however, possible within the scope of the invention. For instance, the properties of the filters may differ, in particular, their suppression frequencies may be non-zero and different from each other. Although FIR filters are preferred, other filters may be used if the variability of the group delay outside the suppression band is sufficiently small. Whereas it is convenient to suppress continuous wave interferers in the order of their ascending frequencies, it is equally possible to suppress them in the order of descending frequencies or in some entirely different order, e.g., according to decreasing strength.

It is, of course, also possible to change the filter characteristics in time, e.g., in order to adapt them to the specific conditions under which the receiver is operating.

LIST OF REFERENCE SYMBOLS

-   1 antenna -   2 radio frequency circuit -   3 band pass filter -   4 TCXO -   5 base band circuit -   6 PLL unit -   7 low noise amplifier -   8 controllable RF amplifier -   9 a,b mixers -   10 a,b high pass filters -   11 a,b low pass filters -   12 a,b variable gain amplifiers -   13 PLL unit -   14 frequency divider -   15 a,b A/D converters -   16 complex mixer -   17 a,b frequency analyzers -   18 control unit -   19 a,b decimation filters -   20 a,b down-samplers -   21 band stop unit -   22 decimator -   23 frequency analyzer -   24 a,b down-samplers -   25 acquisition unit -   26 tracking unit -   27 frequency divider -   28 frequency divider -   29 a-d mixers -   30 a-d band stop filters -   31 a-e numerically controlled oscillators -   32 processing unit -   33 adder -   f₁, f₂, f₃, f₄ interferer frequencies 

1.-17. (canceled)
 18. A method of processing a raw digital signal derived from an analog input signal of a GNSS receiver which is restricted to a fixed raw signal frequency band, the method comprising the following subsequent steps: analyzing the raw digital signal in order to identify continuous wave interferers within the signal frequency band, band stop filtering the raw digital signal by suppressing at least one interferer band containing an interferer frequency of an identified continuous wave interferer to provide a filtered digital signal restricted to a fixed filtered signal frequency band, in that first the raw digital signal is shifted in the frequency domain by the difference between a fixed suppression frequency and the interferer frequency, then a suppression band containing the suppression frequency is suppressed in the shifted digital signal and the shifted digital signal is later shifted to the filtered signal frequency band for providing the filtered digital signal, delivering a series of samples of the filtered digital signal, with successive samples in each case separated by a sampling interval, to a tracking unit (26) where the filtered digital signal is being correlated with internally produced digital sequences characteristic of individual satellites of the GNSS system.
 19. Method according to claim 18, where the raw signal frequency band and the filtered signal frequency band coincide.
 20. Method according to claim 18, the suppression frequency being equal to zero.
 21. Method according to claim 18, where a plurality of interferer bands is suppressed sequentially in that after suppression of a first interferer band containing a first interferer frequency the shifted digital signal is, for every subsequent interferer frequency further shifted in such a way that the shifted interferer frequency coincides with a fixed suppression frequency and then a suppression band containing the suppression frequency is suppressed.
 22. Method according to claim 21, the suppression frequencies being equal.
 23. Method according to claim 21, with the sequence of suppressions of interferer bands following an ascending or descending sequence of the corresponding interferer frequencies.
 24. Method according to claim 18, where the suppression band is suppressed in such a way that at least outside the suppression band delays of different frequency components within the frequency band of the shifted digital signal do not differ by more than half the sampling interval in each case.
 25. Method according to claim 24, suppression of the suppression band being carried out by filtering of the shifted digital signal by a linear phase FIR filter.
 26. Method according to claim 18, where the suppression of the suppression band is carried out by subtracting from each actual value of the shifted digital signal a mean taken over a series of successive previous values of the shifted digital signal.
 27. Method according to claim 26, the mean being in each case taken over a series of fixed length and being replaced by a new mean calculated from a new series following the previous series when the new series is complete.
 28. GNSS receiver base band circuit, with a band stop filter unit configured to filter a raw digital signal contained in a raw signal frequency band to provide a filtered digital signal contained in a fixed filtered signal frequency band, an analyzing unit configured to analyze the raw digital signal in order to identify any continuous wave interferers within the raw signal frequency band, and a tracking unit, the band stop filter unit comprising at least a first band stop subunit with a mixer configured to shift the raw digital signal from the raw signal frequency band by the difference between a fixed suppression frequency and at least a first interferer frequency of a continuous wave interferer, a band stop filter configured to suppress a suppression band containing the suppression frequency of the shifted digital signal and further a mixer configured to shift the shifted digital signal to the fixed filtered signal frequency band.
 29. GNSS receiver base band circuit according to claim 28, where the band stop filter unit comprises a plurality of band stop subunits connected in series.
 30. GNSS receiver base band circuit according to claim 29, where each band stop subunit further comprises a numerically controlled oscillator configured to control the mixer.
 31. GNSS receiver base band circuit according to claim 29, where the band stop filters in the band stop subunits are identical.
 32. GNSS receiver base band circuit according to claim 28, with each band stop filter comprising a processing unit and an adder configured to subtract from the shifted digital signal a processed digital signal derived from the shifted digital signal by the processing unit.
 33. GNSS receiver base band circuit according to claim 32, the processing unit being configured to provide as a processed digital signal a mean of a series of successive values of the shifted digital signal.
 34. GNSS receiver comprising a base band circuit according to claim 28 and further comprising a radio frequency circuit with at least one mixer for providing an analog signal and with at least one A/D converter for converting the analog signal to a digital signal.
 35. Method according to claim 19, the suppression frequency being equal to zero.
 36. Method according to claim 22, with the sequence of suppressions of interferer bands following an ascending or descending sequence of the corresponding interferer frequencies.
 37. GNSS receiver base band circuit according to claim 30, where the band stop filters in the band stop subunits are identical. 